International Journal of Scientific & Engineering Research, Volume 7, Issue 3, March-2016 69 ISSN 2229-5518
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Reduction of Combustion Chamber Heating
by Swirl Shield flow in Liquid Propellant
Rocket Engine Samson PS, Sreemol Balakrishnan, Jerin Cyriac, SarinJose, Rohan Paulose, Leo kJ
Abstract-Ina swirl shield combustion rocket engine theoxidizer is injected tangentially into cylindrical chamber which is
closed at one end and which has a converging outlet at the other end. The flow is introduced into the interior of the
chamber near the outlet end of the chamber and in a direction which is tangent to the inner wall of the chamber. This
tangential injection causes the flow in the chamber to swirl and follow a spiral path up the inner wall of the chamber
and carry away the generating heat due to combustion.
Index Terms-CFD, engine rich exhaust, heat transfer, inner vortex, outer vortex, rocket engine, swirl shield, vertical
helix.
1 INTRODUCTION
THERE are many parts in a rocket, the
Important among them are its payload system,
guidance system, propulsion system, structure
system.The rockets run with combustion
temperatures that can reach ~3500 K (~3227 °C
).Therefore temperatures used in rockets are very
often far higher than the melting point of the
nozzle and combustion chamber
materials(~1200K). Two exceptions are graphite
and tungsten although both are subject to
oxidation if not protected .Here comes the
importance of cooling system in the rocket. If it is
not properly cooled it will be dangerous to the
equipments in it,to the body of the vehicle.so the
temperature should be controlled properly. Indeed
many construction materials can make perfectly
acceptable propellants in their own right. It is
important that these materials be prevented from
Combusting, melting or vaporizing to the point of
failure.
Alternatively, rockets may use more
common construction materials such as
Aluminium, steel, nickel or copper alloys and
employ cooling systems that prevent the
construction material itself becoming too
hot. Regenerative cooling, where the propellant is
passed through tubes around the combustion
chamber or nozzle. Dump cooling (a propellant,
generally hydrogen is passed around the chamber
and dumped), Curtain cooling (propellant injection
is arranged so the temperature of the gases is
cooler at the walls),Film cooling (surfaces are
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wetted with liquid propellant, which cools as it
evaporates).
The object of the present invention is to provide an
improved combustion chamber and method
utilizing the above-described double vortex flow
field. Another object of the present invention is to
provide an improved combustion chamber and
method utilizing the above flow field and to
provide for increased fuel regression rates and
increased travel distance and mixing to achieve
complete combustion. A further object of the
present invention is to provide a liquid rocket
engine utilizing the above-described vortex flow
field. A still further object of the present invention
is to provide an improved hybrid rocket
propulsion system that facilitates and promotes
high and uniform fuel grain regression rates so
that small combustion ports can be used in the
propellant solid grain.
2 WORKING
A liquid rocket engine and a method for
propelling a rocket utilizing a vortex flow field. The
flow field includes an outer fluid vortex spiraling
toward a closed end of the flow field generating
apparatus and an inner fluid vortex substantially
concentric with the outer vortex spiraling away
from the closed end and toward an outlet opening
in which the inner vortex spirals in the same
direction as the outer vortex, but in the opposite
axial direction. The flow field in accordance with
the present invention is capable of providing
separate regions or zones within and among one or
more flowing fluids contained within a common
chamber, without the need for diaphragms or
other physical separators or barriers. Another
embodiment is in the form of liquid rocket engine
to prevent hot combustion products from
contacting the chamber wall.
Virtually countless applications exist for a
flow field Many devices depend upon vortex flows
for their successful operation, such as combustion
chambers, cyclone separators, classifiers and the
like that are in common use. All of these devices
introduce swirling flow at one end of a
passageway in which the flow follows a generally
helical path to exit at the opposite end. Such
conventional vortex flows do not achieve zonal
separation as does the unique flow field that is the
subject of the present invention. it has particular
application to the field of rocket engines and in one
embodiment, specifically to hybrid rocket engines.
Hybrid rocket engines denote a class of rocket
propulsion systems in which one propellant is in
fluid form and the other propellant is in the form
of a solid grain. Typically, the fluid propellant is
the oxidizer and the solid grain is the fuel. The
oxidizer such as liquid oxygen is sprayed into the
combustion ports in the solid fuel grain and caused
to ignite. The hot combustion products sustain the
combustion process until either the oxidizer flow is
shut off or the fuel grain is depleted. The burn rate,
often expressed as regression rate, is the rate at
which fuel can be induced to vaporize the grain
surface so it can participate which provides
separate regions or zones of flowing fluids within a
chamber. There is also a need in the art for a
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combustion chamber and method utilizing such a
flow field, and particularly a combustion chamber
and method for a hybrid rocket engine, which
significantly increases the regression rate of the
solid fuel grain and the effective chamber length
and mixing within the combustion chamber. There
is also a need for a combustion chamber and
method utilizing such a flow field that prevents the
hot combustion products from reaching the
chamber wall.
Figure 1; combustion chamber
In accordance with the present invention, a fluid
flow field, and a structure and method for
producing and sustaining the field, has been
designed. This flow field provides for separate
regions or zones of flowing fluids within a
chamber without the need for physical barriers or
other separators and without substantial mixing
between the regions or zones. In a revolutionary
departure from prior art the present invention
introduces the incoming swirling flow concentric
to the outlet passage and by this means establishes
a new and unique flow field. The flow field
inherently divides into an outer upwardly flowing
vertical helix along a chamber wall, an inner
downward flowing vertical helix along the center
region of the chamber, a converging flow field at
the head end where the outer vortex transforms
into the inner vortex, a converging flow field as the
flow approaches the exit nozzle, and less well
defined regions of velocities and pressure
gradients elsewhere throughout the chamber.
The flow field is produced by injecting
flow tangentially into a cylindrical chamber which
is substantially closed at one end and which has a
converging outlet at the other end. The flow is
introduced into the interior of the chamber near
the outlet end of the chamber and in a direction
which is substantially tangent to the inner wall of
the chamber. This tangential injection causes the
flow in the chamber to swirl and follow a spiral
path up the inner wall of the chamber thereby
establishing an annular vortex flow bounded by
the inner wall of the chamber. When the spiral
flow reaches the closed end of the chamber, the
flow inherently translates inwardly to the center of
the chamber to form the second vortex where the
flow moves spirally away from the closed end,
down the core of the chamber and out the chamber
nozzle. This inner vortex or spiral flow through the
center of the chamber rotates in the same direction
as the outer vortex, pressure at the nozzle
converging wall increases and pressure at the swirl
axis decreases.
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Accordingly, as the inner vortex flow
approaches the nozzle, it enters the converging
section of the nozzle, thereby increasing the swirl
or angular velocity and thus producing an
enhanced radial pressure gradient that blocks the
outflow of the fresh incoming stream .The above-
described flow field has several unique
characteristics. First, the flow path of the injected
fluid before reaching the outlet is quite long and
highly convoluted. Thus, it provides an
opportunity for intense and extensive mixing
along the flow path, particularly in the core or
inner vortex where the angular velocity of the
swirl is greater. Secondly, the outer and inner
vortexes are individually discrete. Thus, the fluid
flow in the inner vortex does not mix significantly
with the fluid flow in the outer vortex.
This enables the inner vortex to support
burning or other chemical reactions to some
significant degree independent of the outer vortex.
Because of this, materials such as propellant or
other chemicals, can be added to the inner vortex
by injection at the conjunction of the two vortices
at the closed end of the chamber and cause
combustion or other chemical reaction to occur and
be sustained wholly in the inner vortex if so
desired The ability to produce and sustain the
above-described double vortex field flow has
countless potential application and several
immediate practical applications.
Object of the present invention is to provide a
hybrid propulsion system that inherently cools the
case walls whenever fuel is not present to insulate
the wall from hot combustion products. A more
specific object of the present invention is to
provide a hybrid rocket propulsion system that
creates and uses a unique internal combustion
vortex flow field to enhance grain regression rate
and to increase the efficiency of the combustion
process. Another object of the present invention is
to provide a combusting flow field that allows the
use of a single grain port for the combustion
process. A further object of the present invention is
to provide an injection means for the fluid
propellant that induces the double vortex flow
field in the grain combustion port. A further object
of the present invention is to provide a combustion
process that inhibits combustion instability.
Another object of the present invention is to
provide a double helix flow field in which an outer
helix flows upwards along the grain surface
inducing combustion, and an inner combustion
helix flows down the port centerline and out the
nozzle to produce thrust.
To achieve the foregoing and other objects and in
accordance with the purpose of the present
invention, a self- contained propulsion system is
provided with a motor casing that houses a solid
propellant grain. A first fluid propellant that will
combust when in the presence of the solid
propellant in the presence of an ignition source, is
stored separately from the solid propellant in a
fluid tank. A delivery means supplies at least a
portion of the said fluid propellant in either liquid
or gaseous state to the combustion port of the solid
grain. An ignition means initiate’s combustion
with the combustion port of the solid propellant
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grain. A fluid injection means that will cause the
fluid propellant to enter the solid propellant grain
case in such a manner as to form an up flowing
helix along the surface of the combustion port in
the solid propellant grain and then a down flowing
helix along the centerline of the combustion port,
said down flowing helix to eventually exit the
chamber via the discharge nozzle.
The fluid propellant can be provided to
the entrance to the fuel grain case by any of
various common means, including delivery from
pressurized tanks, or by pumps of suitable designs.
The fluid can be either the liquid or gaseous state.
Commonly the fluid propellant is the oxidant. In
one embodiment, the oxidant is burned in a highly
oxidizer-rich combustor (termed a "pre-burner")
and the resulting oxidizer-rich combustion
products are used to drive a turbo pump that
pressurizes the liquid oxidizer for delivery to the
pre-burner. After driving the turbine, the oxidizer-
rich combustion products leave the turbine and
flow to the injection ports of the fuel grain high
pressure casing.
The oxidant enters the fuel grain ports in a
fluid phase that may be at high enough pressure to
be supercritical. The injector elements are
positioned and designed such that the injected
flow develops the co-axial vortex flow field within
the chamber in the manner that is the subject of
this invention. In another embodiment, the
oxidizer in liquid state is carried in a high pressure
tank. Pressure is supplied by a conventional tank
pressurization system well known to those
acquainted with the profession. The liquid oxidant
is expelled from the tank and delivered at high
pressure to the injection ports of the fuel grain high
pressure casing.
2.1 Combustion Chamber
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Figure 2; Dimensions of combustion chamber.
This is the bottom view of the combustion
chamber .diameter for each holes are shown in the
diagram itself. All dimensions are in mm.
2.2 Fuel Injector
Figure 3; Fuel injector
This is the figure of the fuel injector where
fuel is injected into the combustion chamber. It
consists of small minute holes in order to get
maximum atomization of the fuel. The holes are
inclined in such a way that it enables the fuel to
coincide at the center ,which help to strike the fuel
coming from each holes at center and splash it to
get the maximum atomization.
Solid Works Flow Simulation uses Computational
Fluid Dynamics (CFD) analysis to enable quick,
efficient simulation of fluid flow and heat transfer.
Inlet mass flow rate of fuel is 0.3 lb/sec, which is
indicated on the top portion of the combustion
chamber, inlet mass flow rate of the oxidizer is
0.547lb/sec and the outlet environment pressure is
101325 Pascal.
3 RESULT
First, the high velocity outer vortex scrubs
the burning fuel grain surface, causing enhanced
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heat transfer to the surface. Combustion near and
on the surface is also able process because fresh
oxidizer is carried directly to the surface by
turbulent transport mechanisms in addition to the
usual molecular diffusion process. Second, the
vortex also sustains radial pressure and density
gradients that cause hot, low density combustion
products to be buoyed out of the combustion zone
so their presence does not hinder the combustion
process. Third, because the flow path of the
injected fluid (the oxidizer) to reach the outlet is
very long and highly convoluted, it provides an
opportunity for intense and extensive mixing and
combustion with the fuel grain vapor, particularly
in the core or inner vortex. Accordingly, in the
above application, the outer vortex flow causes
rapid burning of the fuel grain on the wall of the
cylinder, and the inner vortex causes combustion
to proceed rapidly, by providing intense mixing
and combustion travel distance to allow
combustion to reach completion, thereby achieving
high combustion efficiency.
3.1 Visualizing Results
After running the analysis, the software
generates customizable default result plots.
Other plots can also be defined by right-
clicking a result folder and selecting Define. When
defining plots, you can use reference coordinate
systems. For example, you can view radial and
tangential stresses by selecting an axis when
defining stress plots. You can associate result plots
with named views.
Result viewing tools include fringe plots,
section plots, iso plots, animation, probing, and
exploded views. For sections plots, you can choose
planar, cylindrical, and/or spherical cutting tools.
A clipping utility is provided for convenient
viewing of section and iso plots.
Solid Works Flow Simulation provides advanced
easy-to use tools to visualize the results: Cut, 3D-
Profile and Surface Plots (contours, isolines, and
vectors), Isosurfaces, XY plots, Flow and Particle
Trajectories, Animation of Results. Solid Works
Flow Simulation provides advanced tools to
process the results: Point, Surface and Volume
Parameters, Plots of Goals, MS Word Report.
This figure below shows the temperature
distribution inside the combustion chamber. The
temperature is varied at each place in the
combustion chamber. From the figure it is clear
that the temperature at the wall of the combustion
chamber is considerably low. High temperature is
obtained at the core portion as well as at the top of
the combustion chamber. The table at the left side
of the figure shows the variation of temperature
along the combustion chamber. Near the wall of
the combustion chamber a very low temperature is
developed, which is seen in green color in the
figure.
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Figure 4: temperature distribution inside the
combustion
The high intense temperature is at the
core, which has red color. When the flow comes to
exit its temperature is considerably low and having
a color of blue. From this figure we can understand
that the wall of the combustion chamber is
protected from developing a high temperature by
the swirl shield effect. So here the prevention of
generating heat in the combustion chamber wall is
done rather than curing it after the heat generation.
The temperature value of each color is indicated in
the left side table.
Figure 5: velocity distribution inside the combustion
In the above figure, the velocity distribution of
oxidizer flow inside the combustion chamber .The
corresponding values of velocity for different
colors is shown in the left side table. The velocity
of oxidizer at the outer vortex is different from that
of inner vortex. The outer and inner vortexes are
represented in sky-blue and dark blue color
respectively. At the throat region velocity is
reaches to match velocity, which can be identified
by the color and velocity value combination from
the table. Because of the convergent divergent
nozzle the velocity of flow after the throat is
supersonic; this is represented by the red color
flow lines. The arrow marks on each flow line
shows its direction.
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Figure 6: temperature distribution inside the
combustion
This figure shows the temperature
distribution of the gas flow lines, inside the
combustion chamber. The temperature is reduced
when it goes from top to bottom and also towards
the core region from the periphery. The intensity of
temperature is increased from the blue color to red
color, which is shown in the left table. The arrow
mark on each flow line indicates its direction.
3.2Experimentaltest
At the time of ignition
After 5 seconds
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After 15 seconds
after 30 seconds
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4 CONCLUSION
The present invention relates generally to a vortex
flow field and the apparatus and method to
produce and sustain it and more particularly to a
hybrid rocket engine and a method of propelling a
rocket utilizing such vortex flow field. The flow
field in accordance with the present invention is
capable of providing separate regions or zones
within and among one or more flowing fluids
contained within a common chamber, without the
need for diaphragms or other physical separators
or barriers. It is evident and believed that the flow
field of the present invention has utility to a wide
range of applications. One general field of
application is that of combustion chambers, and
more particularly, that of combustion chambers
and methods for rocket engines or the like and
hybrid rocket propulsion systems. A combustion
chamber and method in accordance with one
embodiment of the present invention utilizes the
unique flow field of the present invention to
improve hybrid rocket fuel regression and increase
mixing length in a rocket or other engine. Another
embodiment is in the form of liquid rocket engine
to prevent hot combustion products from
contacting the chamber wall. By this new
innovative idea we developed a new rocket engine
which has 20% weight reduction than the
conventional rocket engine. This is accomplished
by avoiding the extra cooling mechanism that is
used in conventional engines. Here we prevent the
formation of heat on the wall of the combustion
chamber rather than cooling it after it become hot.
ACKNOWLEDGMENT
I gratefully remembers the contribution made by
Sarin Jose, Rohan Paulose, Leo kJ 2013 batch
students of VJECfor their contribution in this
project and for giving me the permission to present
the paper. Also humbly acknowledges the
contribution of Prof. Jerin Cyriac, the professor of
mechanical engineering, at Vimal Jyothi
engineering college, Chemperi, for the great
contribution he had done to this project and also
for guiding me from the beginning to the end.
REFERANCE
1. 1. Aerospace Propulsion, by Dennis G. Shepherd,
Elsevier Publishing Company, 335 Vanderbilt Avenue,
New York, NY, 1972 . ISBN 71-190302.
2. 2 Rocket Propulsion Elements, by George P. Sutton.
John Wiley & Sons, Inc., New York, 1964.
3. 3 Design of Liquid, Solid, and Hybrid Rockets, by R. L.
Peters. Hayden Book Co. Inc., New York, 1965.
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